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Terahertz quantum beats in molecular liquids

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In this paper, the femtosecond time resolution of the experiment allows the study of pronounced high-frequency beat phenomena up to 10 THz, and the frequency difference between vibrational modes separated by more than 300 cm−1 may be determined with high precision.
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This article is published in Chemical Physics Letters.The article was published on 1987-01-30 and is currently open access. It has received 165 citations till now. The article focuses on the topics: Quantum beats & Femtosecond.

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Citations
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Single-pulse coherently controlled nonlinear Raman spectroscopy and microscopy

TL;DR: This work performs single-pulse vibrational spectroscopy on several molecules in the liquid phase, where both the excitation and the readout processes are performed by the same pulse, using a single broadband laser source.
Journal ArticleDOI

A large-cavity zeolite with wide pore windows and potential as an oil refining catalyst

TL;DR: The synthesis of ITQ-21 is reported, a zeolite with a three-dimensional pore network containing 1.18-nm-wide cavities that exhibits high catalytic activity and selectivity for valuable products in preliminary oil refining tests.
Journal ArticleDOI

Femtosecond optical Kerr studies on the origin of the nonlinear responses in simple liquids

TL;DR: In this article, the time-resolved optical Kerr responses of several simple molecular liquids are probed with 65-fs laser pulses and four dynamically distinct responses associated with the nonlinear susceptibility are observed in every liquid that possesses a permanent anisotropic polarizability.
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Optimizing the laser-pulse configuration for coherent Raman spectroscopy.

TL;DR: A hybrid technique that combines the robustness of frequency-resolved coherent anti-Stokes Raman scattering (CARS) with the advantages of time-resolving CARS spectroscopy is introduced and a rapid and highly specific detection scheme that works even in the presence of multiple scattering is demonstrated.
Journal ArticleDOI

Coherent anti-Stokes Raman Scattering Microscopy

TL;DR: Results show that CARS microscopy has the potential to become an important complementary technique that can be used with other well-established microscopic methods, and it can be expected that the impressive growth of the field will continue.
References
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Journal ArticleDOI

Vibrational dynamics of liquids and solids investigated by picosecond light pulses

TL;DR: In this article, a detailed theoretical treatment of different excitation and probing processes are outlined and a variety of results are presented and discussed, including the population lifetime of known vibrational modes and evidence for inter-and intra-molecular interactions.
Journal ArticleDOI

Molecular Vibrations in Liquids: Direct Measurement of the Molecular Dephasing Time; Determination of the Shape of Picosecond Light Pulses

TL;DR: In this paper, the dephasing time of a light pulse was obtained when the vibrational amplitude is coherently excited by an intense light pulse of duration (t) of length (p).
Journal ArticleDOI

Time resolved observation of resonant and non-resonant contributions to the nonlinear susceptibility χ(3)

TL;DR: In this article, the resonant and nonresonant part of χ(3) are distinguished by their different time behavior, and the medium is coherently excited by two picosecond light pulses of defined frequency difference.
Journal ArticleDOI

Generation of femtosecond light pulses in the near infrared around λ = 850 nm

TL;DR: In this paper, a synchronously pumped ring dye laser was used to produce femtosecond light pulses tunable between 840 nm and 880 nm, with pulse durations down to 65 fs.
Journal ArticleDOI

Quantum beating of vibrational factor group components in molecular solidsa)

TL;DR: In this article, the first coherent Raman induced quantum beats from exciton states in molecular crystals were observed in C6H6 at 1.6 K. The authors described the relevant crystal optics and phasematching conditions needed to ensure coherent excitation of more than one Raman transition in an anisotropic solid.
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Frequently Asked Questions (20)
Q1. What have the authors contributed in "Terahertz quantum beats in molecular liquids r. leonhardt, w. holzapfel, w. zinth and w. raiser" ?

Femtosecond pulses allow us to investigate the decay dynamics of vibrational transitions with dephasing times T, of less than 1 ps and provide the possibility to study fast beating phenomena on a frequency scale of many terahertz. Time-resolved coherent Raman scattering is commonly treated under the following assumptions: The authors limit the discussion to polarized Lorentzian-shaped Raman lines. 

In this Letter the application of femtosecond pulses to coherent Raman spectroscopy of molecular transitions in liquid systems is discussed. 

A major advantage of the system is the ready tunability of the excitation frequency wL- ws using the birefringent filter of thepicosecond laser. 

Due to the broad spectral widths of the femtosecond exciting force of Aw/27co 200 cm-’ both pyridine modes are simultaneously excited in the experiment. 

The authors found three peaks in the Fourier spectrum at 39,189, and 228 cm-‘, which correspond to the frequency differences between the three modes excited in their mixture. 

The coherent signal S, is recorded as a function of the delay time (set by the optical delay line VD) between the exciting and probing pulses EL and EL*, respectively. 

The length of the unidirectional ring laser is actively controlled in order to synchronize the pulses from the femtosecond and the picosecond laser with temporal jitter of less than 5 ps. 

The driving force F(x,t) for the coherent amplitude Q is0 009-2614/87/$03.50 0 Elsevier Science Publishers B.V. (North-Holland Physics Publishing Division)373proportional to the product of the laser and Stokes fields, F(x,t) a E=a. 

The pulses from this laser provide the exciting and probing light fields EL and EL*, respectively with an average power of z 10 mW. 

Two modes separated by= 189 cm-’ are excited simultaneously, leading to the observed beat frequency of 5.7 THz.esting features are seen at early delay times. 

(5)The authors assume T2, > T,,. From eq. (5) it is evident that the coherent signal consists of a sum of three contributions multiplied by the factor exp( -2tD Ty,‘) (the exponential decay can be removed from measured coherent data by multiplication with exp( 2tDTy,’ )). 

The coherently scattered light field consists of a sum over contributions originating from the differentvibrational modes j:2&S(tD)a cQJ(b> exp(-iwwtD+k$i) . (4) JThe evolution of the coherent signal is readily demonstrated for the case of two molecular transitions at frequencies w, and w,+Sw. 

one observes the scattered energy S, at the end of the sample, which is proportional to the time-integrated intensity, i.e. &s( tD) aJdt The authorEAs( t,tD) ) *.For sufficiently short exciting and probing pulses, t, < T2, and for late delay times, t+ tp, the salient features of the coherent signal are: (i) For a single vibrational mode the signal decays exponentially with exp( - 2tdT2). 

In a time-resolved coherent Raman experiment the coherent amplitude (q) which is generated at time zero is monitored by coherent Raman scattering of a delayed probing pulse EL2. 

The anti-Stokes radiation EAs generated by the probing process passes the second polarizer and is detected after the broad-band spectrometer SP by the cooled photomultiplier PM. 

3 the authors show the decay of the coherent antiStokes signal recorded from the binary mixture of cyclohexane and benzene of 1: 1 by volume. 

The vibrational excitation of an ensemble of molecules is described by the expectation value of the vibrational amplitude (q) = 4iQ exp( -io, t+ik, x) +c.c. 

The application of linear response theory to the excitation process leads to the following equation for the coherent amplitude Qj [ 1 ] :fQ, ew(i@,,) =K, s dt’ EL(f) B(f) --mxexp[(t’-t)lTz,] exp[ -iAw,t’] . 

The frequency of the exciting force was set to 900 cm- ’ in order to excite simultaneously Raman-active transitions in cyclohexane at 802 cm- ’ and in benzene at 992 cm-‘. 

The total vibrational excitation may be described as the superposition of the individual states ( qj) with well defined amplitudes Q,, frequencies o, , and phase factors @,I:(4) =C<%) j=tiFQ, exp( - io,t+ik,x+i&) +c.c. (1)The coherent amplitude of a Raman-active mode with frequency oti can be excited via transient stimulated Raman scattering [ 91 by a pair of light pulses, the laser pulse EL, and the Stokes pulse Es.